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Find the Green's function for the boundary value problem
given that is a fundamental set of solutions of
the complementary equation. Then use the
Green's function to solve (A) with (a) and (b) .
Short Answer
Expert verified
Answer:
For :
For :
Step by step solution
01
Complementary equation solution
From the information given, we know that is a fundamental set of solutions to the complementary equation. So, the general solution of the complementary equation is
Since it is a boundary value problem, we need to consider our boundary conditions for .
02
Apply boundary conditions
Apply the given boundary conditions and to the general solution.
and
03
Find Wronskian
In order to find the Green's function, we need to find the Wronskian of the fundamental set of solutions. The Wronskian is defined for our two given functions as
04
Green's function
Now we can write the Green's function as
Replacing , , and , we obtain
05
Solve for given
Finally, we can use the Green's function to solve the boundary value problem for the given functions:
(a) For , the particular solution is given by
Split the integral based on the Green's function:
Simplify the integrals and evaluate them:
(b) For , the particular solution is given by
Split the integral based on the Green's function:
Simplify the integrals and evaluate them:
In conclusion, we have found the particular solutions for the given functions, and they are:
for , and
for .
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Boundary Value Problem
A boundary value problem is a differential equation with conditions specified at the boundaries of the interval on which the solution is defined. These problems often occur in various fields such as physics, engineering, and mathematics. In our original exercise, we deal with the differential equation . The boundary conditions are and . These conditions mean we seek a solution that satisfies the differential equation within the interval [1, 2] and simultaneously meets the conditions at and . Boundary value problems can have unique solutions, no solutions, or infinite solutions depending on the feature of the differential equation and the boundary conditions applied. In this exercise, we identify the complementary equation and then use its solutions to form the Green's function, broadening our approach to solve the boundary value problem.
Complementary Equation
The complementary equation is a part of the solution process for non-homogeneous linear differential equations. It involves finding solutions to the associated homogeneous equation . These solutions help us generate a general solution for the original differential equation. The exercise tells us that forms a fundamental set of solutions for the complementary equation, leading to a general solution of . These solutions play a crucial role in building both the homogeneous solution and the particular solution to the boundary value problem. In practical terms, solutions to the complementary equation are used to form a general solution that is adjusted to satisfy individual boundary conditions.
Wronskian
The Wronskian is a determinant used to test if a set of solutions to a differential equation is linearly independent, which means none of the solutions can be formed by a combination of the others. In our case, the Wronskian is calculated for the solutions and . The Wronskian is determined as:
This simplifies to:
By calculating the Wronskian, we ascertain the linear independence of and . This independence implies that indeed forms a fundamental solution set necessary for constructing the Green’s function for the boundary value problem.
Particular Solution
A particular solution is a specific solution to a non-homogeneous differential equation, serving as one component of the complete solution when combined with the general solution of the complementary equation. In steps 5(a) and 5(b) of the solution, the particular solution is determined using the Green’s function. For function , the integral involves and gives a result of: For , the associated particular solution derived from the Green’s function is: These series of calculations demonstrate how specific source terms change the output of the particular solution, showcasing the flexibility of Green’s function in solving complex boundary value problems.
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